沟谷泥石流危险度计算公式的由来及其应用实例

首先介绍了本文作者提出的最新单沟泥石流危险度定量评价计算公式的由来,包括单沟泥石流危险度评价因子的选择,即主要因子的确定和次要因子的筛选,明确了各评价因子的作用,用权重系数方式表达各评价因子对泥石流危险度的影响。然后以2003年发生的四川省丹巴县鹅狼沟泥石流为例,对该沟泥石流危险度进行了定量评价,结果表明其为高度危险的泥石流沟。最后讨论了泥石流危险度计算的经验公式和理论公式及可能遇到的有关问题。     

2021年11月17日江苏大丰海域MS5.0地震震源深度对比分析

选取江苏测震台网震中距2°以内18个地震台站记录清晰的波形资料,使用单纯形、LocSAT、HypoSAT地震定位方法,分别采用华南速度模型、郯庐断裂带中南段速度模型以及IASP91全球速度模型,重新测定江苏大丰海域M_S5.0地震震源深度,对获取的深度值进行对比分析。结果表明:3种地震定位方法测定的震源深度结果接近,约为11 ± 2 km;HypoSAT定位方法计算结果较为稳定,IASP91、郯庐断裂带中南段模型均适用于该区域震源深度计算。      

二滩水电站地震遥测台网持续时间震级的研制

利用二滩水电站地震遥测台网的速度量和位移量观测记录,收集了震级ＭＬ为０．４￣５．４的４６０次地震（Δ〈２１０ｋｍ）的振动持续时间３５００多条,制作了该台网的持续时间震级公式和便查表。在方法上,不同于通常的按一次或两次曲线拟合,而采取计算机自动分段按折线拟合的方法,以阻尼最小二乘法完成其计算;在资料上,先分台制作８个子台的持续时间震级公式,在此基础上选择仪器、台基及公式中参数相近的子台,制作了适用于     

设置芯柱-构造柱混凝土砌块墙体抗震剪切承载力计算

本文收集了国内大量的混凝土小型空心砌块墙片试验资料,通过研究芯柱一构造柱混凝土小型空心砌块组合砌体受力特征及影响抗震剪切承载力的主要因素,结合理论计算分析,提出了抗震剪切承载力的通用计算公式。该公式既适用于芯柱-构造柱混凝土小砌块墙体,又适用于只设置芯柱或构造柱砌块墙体结构。通过试验值与计算值的比较,证明本文所提出通用公式的准确性。     

反应谱对构造环境剪应力场的依赖性

在以前理论工作的基础上, 导出了构造环境剪应力值对反应谱的影响. 在美国知名学者Boore等建立的预测公式BJF94的基础上, 提出了新的预测公式CLB20. 在CLB20中引进了应力场量值tau;0对SA的影响项. BJF94主要是基于美国西部的强震观测资料作出的经验预测公式, 而SEA99是基于全球张性地区的强震观测资料作出的预测公式. 我们把两者的预测结果进行了全面的比较, 发现BJF94的预测值lg(Y) 减去0.16个对数单位后, 与SEA99的预测值十分接近. 这说明张性地区的 lg(Y) 较小; 地区性差异主要表现在构造环境剪应力场的差异上. 如果这个因素在预测公式中能得到适当体现, 同时预测公式中的震级标度都用全球统一的矩震级, 距离都使用多数人倾向使用的断层投影距, 那么预测公式的地区性差异将大大减轻, 以至最后消失, 有可能构造出全球适用的预测公式. 我们的抗震设计直接引用美国研究者发表的反应谱衰减结果（例如BJF94和SEA99）, 不会导致太大的误差.       

区域综合地震数据库系统研制过程中的几点技术措施

本文介绍的区域综合地震数据库系统,通过采取一定的技术措施,不仅具有一般应用软件模块化的程序结构、通用性及可移植性强、设计简洁明快、用户界面友好以及容错纠错功能强等特点,而且研制出了记忆性(智能化)的录入模块,用于大量地震资料的录入,可成倍提高工作效率;在按台项建立子库的基础上,采用等分算法进一步实现了快速检索功能,该功能不论是对于等时间间隔序列还是对于不等时间间隔序列的观测资料,都能提高查询速度数倍。这些方法不仅适用于地震数据管理,同样适用于其它行业类似的大量的资料管理和查询。     

玉树MS7.1级地震前的形变应变场变化特征

基于1999～2007年和2007～2009年的GPS站点观测数据计算的速度场,分析了青藏亚板块的运动特征.利用块体(旋转与线性应变)弹性运动公式计算可可西里-巴颜喀拉块体和羌唐块体的应变率、可可西里-玉树断裂带的运动速度和应变率,研究了玉树7.1级地震前的形变应变特征.结果表明:可可西里-巴颜喀拉块体处于青藏亚板块运...     

中国历史大地震的矩震级

本文把地震矩和地面加速度之间的理论关系与地震烈度和该加速度之间的经验关系结合起来,导出了使用Ⅵ度等震线平均半径估算我国历史大地震矩震级的公式。 我们使用这一公式给出了53个大地震的矩震级,并对其它震源参数作了计算和讨论。从本文的结果来看,板内地震的矩震级不大于9.0。     

二维频率空间域粘声波正演模拟研究

地球介质本身的非弹性导致大地吸收效应,黏滞性影响波场的所有频率成分且对高频成分的影响更大,从而降低了地震记录和地震成像的垂向分辨率.通常使用经验公式描述吸收衰减.在时间域模拟吸收衰减需大量的计算机内存、计算效率较低,模拟Q值非常困难;而频率空间域可以通过引入复速度和Q值,使用任意的经验公式而进行粘滞介质的数值模拟.本文...     

福州地震台P2000测氡仪试测实验分析

对P2000与FD-125测氡仪进行为期一个半月的同步观测对比,并对P2000测氡仪该装置是否适用于地震氡观测及氡气标定器的刻度校正进行测试实验,根据观测的数据进行归纳和总结.结果表明,P2000测氡仪稳定性较好,操作使用简单,一次性充电可以连续使用十几个小时,较适用于野外观测.缺点是该测氡1次只能测1个水样,如果要测两平行样要六七个小时,时间相对较长.对观测的数据对比分析,发现虽然P2000测氡仪测值低于FD-125氡钍分析器的测值,但整体形态和趋势变化基本一致.     

CONCENTRATION AND VELOCITY OF DEBRIS FLOWS

1 RESISTANCE TO WATER-STONE FLOW As a special sort of debris flow, water-stone flow, or as generally called, sub-viscous debris flow, always occurs in channel of steep slope, dominantly in composition of coarse grains of bedload and laminated load with less suspended load. In some literature, water-stone flow is defined for convenience of study as that without suspended fine grains in composition, and it follows from this definition that transportation concentration of this kind of …     

GIS‐assisted modelling for debris flow hazard assessment based on the events of May 1998 in the area of Sarno,Southern Italy: II. Velocity and dynamic pressure

The velocity and dynamic pressure of debris flows are critical determinants of the impact of these natural phenomena on infrastructure. Therefore, the prediction of these parameters is critical for hazard assessment and vulnerability analysis. We present here an approach to predict the velocity of debris flows on the basis of the energy line concept. First, we obtained empirically and field‐based estimates of debris flow peak discharge, mean velocity at peak discharge and velocity, at channel bends and within the fans of ten of the debris flow events that occurred in May 1998 in the area of Sarno, Southern Italy. We used this data to calibrate regression models that enable the prediction of velocity as a function of the vertical distance between the energy line and the surface. Despite the complexity in morphology and behaviour of these flows, the statistical fits were good and the debris flow velocities can be predicted with an associated uncertainty of less than 30% and less than 3 m s^?1. We wrote code in Visual Basic for Applications (VBA) that runs within ArcGIS^® to implement the results of these calibrations and enable the automatic production of velocity and dynamic pressure maps. The collected data and resulting empirical models constitute a realistic basis for more complex numerical modelling. In addition, the GIS implementation constitutes a useful decision‐support tool for real‐time hazard mitigation. Copyright © 2008 John Wiley & Sons, Ltd.     

Bed scour by debris flows: experimental investigation of effects of debris‐flow composition

Debris flows can grow greatly in size by entrainment of bed material, enhancing their runout and hazardous impact. Here, we experimentally investigate the effects of debris‐flow composition on the amount and spatial patterns of bed scour and erosion downstream of a fixed to erodible bed transition. The experimental debris flows were observed to entrain bed particles both grain by grain and en masse, and the majority of entrainment was observed to occur during passage of the flow front. The spatial bed scour patterns are highly variable, but large‐scale patterns are largely similar over 22.5–35° channel slopes for debris flows of similar composition. Scour depth is generally largest slightly downstream of the fixed to erodible bed transition, except for clay‐rich debris flows, which cause a relatively uniform scour pattern. The spatial variability in the scour depth decreases with increasing water, gravel (= grain size) and clay fraction. Basal scour depth increases with channel slope, flow velocity, flow depth, discharge and shear stress in our experiments, whereas there is no correlation with grain collisional stress. The strongest correlation is between basal scour and shear stress and discharge. There are substantial differences in the scour caused by different types of debris flows. In general, mean and maximum scour depths become larger with increasing water fraction and grain size, and decrease with increasing clay content. However, the erodibility of coarse‐grained experimental debris flows (gravel fraction = 0.64) is similar on a wide range of channel slopes, flow depths, flow velocities, discharges and shear stresses. This probably relates to the relatively large influence of grain‐collisional stress to the total bed stress in these flows (30–50%). The relative effect of grain‐collisional stress is low in the other experimental debris flows (<5%), causing erosion to be largely controlled by basal shear stress. Copyright © 2016 John Wiley & Sons, Ltd.     

Experimental analysis on the impact force of viscous debris flow

A miniaturized flume experiment was carried out to measure impact forces of viscous debris flow. The flow depth (7.2–11.2 cm), velocity (2.4–5.2 m/s) and impact force were recorded during the experiment. The impact process of debris flow can be divided into three phases by analyzing the variation of impact signals and flow regime. The three phases are the sudden strong impact of the debris flow head, continuous dynamic pressure of the body and slight static pressure of the tail. The variation of impact process is consistent with the change in the flow regime. The head has strong–rapid impact pressure, which is shown as a turbulent‐type flow; the body approximates to steady laminar flow. Accordingly, the process of debris flows hitting structures was simplified to a triangle shape, ignoring the pressure of the tail. In order to study the distribution of the debris flow impact force at different depths and variation of the impact process over time, the impact signals of slurry and coarse particles were separated from the original signals using wavelet analysis. The slurry's dynamic pressure signal appears to be a smooth curve, and the peak pressure is 12–34 kPa when the debris flow head hits the sensors, which is about 1.54 ± 0.36 times the continuous dynamic pressure of the debris flow body. The limit of application of the empirical parameter α in the hydraulic formula was also noted. We introduced the power function relationship of α and the Froude number of debris flows, and proposed a universal model for calculating dynamic pressure. The impact pressure of large particles has the characteristic of randomness. The mean frequency of large particles impacting the sensor is 210 ± 50–287 ± 29 times per second, and it is 336 ± 114–490 ± 69 times per second for the debris flow head, which is greater than that in the debris flow body. Peak impact pressure of particles at different flow depths is 40–160 kPa, which is 3.2 ± 1.5 times the impact pressure of the slurry at the bottom of the flow, 3.1 ± 0.9 times the flow in the middle, and 3.3 ± 0.9 times the flow at the surface. The differences in impact frequency indicate that most of the large particles concentrate in the debris flow head, and the number of particles in the debris flow head increases with height. This research supports the study of solid–liquid two phase flow mechanisms, and helps engineering design and risk assessment in debris flow prone areas. Copyright © 2015 John Wiley & Sons, Ltd.     

VOLUMETRIC SEDIMENT CONCENTRATION IN DEBRIS FLOWS

1　ＩＮＴＲＯＤＵＣＴＩＯＮ　Ｄｅｂｒｉｓｆｌｏｗｓｏｃｃｕｒｗｈｅｎｒａｉｎｓｔｏｒｍｓｏｒｔｈｅｅｌｅｖａｔｉｏｎｏｆｕｎｄｅｒｇｒｏｕｎｄｗａｔｅｒｌｅｖｅｌｃａｕｓｅｌｏｏｓｅｄｅｐｏｓｉｔｓｏｒｐｅｔｒｉｆｉｅｄｏｂｊｅｃｔｓｓｕｃｈａｓｐ?..     

RELATION BETWEEN PRECIPITATION AND INITIATION OF DEBRIS FLOWS IN THE JIANGJIA RAVINE,YUNNAN PROVINCE, SOUTHWEST CHINA

1 INTRODUCTION In the watershed of the Jiangjia Ravine, the frequency of occurrence of rainstorms which can mobilize debris flows is high, and there are abundant unconsolidated materials deposited in the upstream area, these resulted in frequent eruption …     

EXPERIMENTAL STUDY OF BEDLOAD TRANSPORT IN UNSTEADY OPEN-CHANNEL FLOW

I.INTRODUCTIONBedloadtransportinsteadyuniformopenchannelflowhasbeenextensiVelystudied.Manyoftheformulasdevelopedforthepredictionofbedloadtransportinuniformopen-channelflowcanbebroughtinthefollowingform(ChienandWan,1983);ac=f(O)(l)xvhereacisthedimensionlessparameterofbedloadtranSPortandOisthedimensionlessparameterofflowintensity.TheseparametersaredefinedasfwheregsisthebedloadtranspoftratePerunitwidthindryweight;disthesedimentdiameter,Sisthebedslopeofthechannel;Rbisthehydraulicradiusdue…     

Erosion and deposition by debris flows at Mt Thomas,North Canterbury,New Zealand

The grass-covered slopes on the southern flank of Mt Thomas, an upfaulted block of highly sheared sandstone and argillite 40 km NW of Christchurch, New Zealand, are presently undergoing severe erosion by a combination of mass-wasting processes. Gully erosion, soil slips, and debris flows have carved out a number of steep, deeply incised ravines, from which coarse debris is transported (primarily by debris flows) to alluvial fans below. Geologic and historical evidence indicates that debris flows have been episodically active here for at least the last 20,000 years and have been the dominant process in fan building. This demonstrates that catastrophic geomorphic processes, rather than processes acting at relatively uniform rates, can be dominant in humid-temperate areas as well as in arid and semi-arid regions. In April 1978, debris flows were triggered in one of two unstable ravines in the Bullock Creek catchment by a moderate intensity, long duration rainstorm with a return period in excess of 20 years. Surges of fluid debris, moving at velocities up to 5 m/s, transported a dense slurry of gravel, sand, and mud up to 3·5 km over a vertical fall of 600 m. Deposition on the alluvial fan occurred when the flows left the confines of an entrenched fan-head channel and spread out as a 0·16 km² sheet averaging 1·2 m thick. In all, 195,000 m³ were deposited, roughly a third of that being reworked sediments from the head of the fan. Sediment yield from this one event would be equivalent to several thousand years worth of erosion at average sediment discharge rates for small South Island mountain catchments. Samples of viscous fluid debris during surges contained up to 84 per cent solids, composed of 70 per cent gravel, 20 per cent silt, and 4 per cent clay. Fluid density of the material ranged between 1·95 and 2·13 g/cm³, and it was extremely poorly sorted. Between surges the fluid was less viscous, less dense, and unable to carry gravel in suspension. Severe fan-head entrenchment of the stream channel (approximately 10 m in less than 24 hours) was accomplished by the erosive action of the surges. Tectonic uplift of the Mt Thomas block and the weak, crushed condition of the bedrock appear to be ultimately responsible for the catastropic erosion of slopes in the Bullock Creek catchment. However, forest clearing within the last few centuries appears to have greatly increased the rate of mass wasting and gully erosion on these slopes.     

格栅坝在泥石流防治中的应用——以汶川地震引发的烂泥沟泥石流治理为例

受汶川地震影响,四川等地泥石流治理更为迫切。泥石流的暴发具有突发性,在防治工程中,相比实体坝而言,格栅坝是一种节省材料、稳定性更高的拦挡结构,使用范围越来越广,但是目前尚无成熟的格栅坝设计方法。本文参考梳齿坝的已有理论确定了支墩间距的计算方法,并结合已有实验资料提出了格栅坝格栅间距的计算公式,改变了以往不同坝体乃至同一坝内各横梁间距一致的计算方法。另外,因支墩间隔相对较小,以简支模式计算石块对横梁冲击力并不合适,本文基于固定梁模式重新推导了计算公式,其计算结果与简支梁模式比较,数值大了3倍。最后考虑坝体建成后的不同情况,提出了支墩、横梁及两侧翼墙的详细计算工况,并基于以上设计理论,对烂泥沟泥石流治理工程的部分格栅坝进行了具体设计。     

Experimental study of debris flow caused by domino failures of landslide dams

The formation of landslide dams is often induced by earthquakes in mountainous areas.The failure of a landslide dam typically results in catastrophic flash floods or debris flows downstream.Significant attention has been given to the processes and mechanisms involved in the failure of individual landslide dams.However,the processes leading to domino failures of multiple landslide dams remain unclear.In this study,experimental tests were carried out to investigate the domino failure of landslide dams and the consequent enlargement of downstream debris flows.Different blockage conditions were considered,including complete blockage,partial blockage and erodible bed（no blockage）.The mean velocity of the flow front was estimated by videos.Total stress transducers（TSTs）and Laser range finders（LRFs） were employed to measure the total stress and the depth of the flow front,respectively.Under a complete blockage pattern,a portion of the debris flow was trapped in front of each retained landslide dam before the latter collapsed completely.This was accompanied by a dramatic decrease in the mean velocity of the flow front.Conversely,under both partial blockage and erodible bed conditions,the mean velocity of the flow front increased gradually downward along the sloping channel.Domino failures of the landslide dams were triggered when a series of dams（complete blockage and partial blockage） were distributed along the flume.However,not all of these domino failures led to enlarged debris flows.The modes of dam failures have significant impacts on the enlargement of debris flows.Therefore,further research is necessary to understand the mechanisms of domino failures of landslide dams and their effects on the enlargement of debris flows.